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How High Can You Jump On Mars?
How High Can You Jump On Mars?

... where v is the linear speed of the object along the circular path and R is the radius of the circle. Remembering Newton's second law, we can multiply both sides of this equation by the mass of the object to nd the force being applied to the object: ...
biomechanics of combatives and an analysis of work and power
biomechanics of combatives and an analysis of work and power

Document
Document

Physics Unit 2 Review
Physics Unit 2 Review

... Identify the choice that best completes the statement or answers the question. 1. The SI unit of force is the a. joule. c. meter. b. kilogram. d. newton. 2. When an unbalanced force acts on an object, a. the object’s motion does not change. c. the weight of the object decreases. b. the object accele ...
Newton`s Second Law (F=ma)
Newton`s Second Law (F=ma)

... Fill in the blank with the appropriate term. 1. __________ occurs whenever an object is acted upon by an unbalanced force. 2. The acceleration of an object is determined by the net force acting on the object and the object’s __________. 3. Newton’s second law of motion shows that there is a direct r ...
Work and Energy LESSON OBJECTIVES Students will be able to
Work and Energy LESSON OBJECTIVES Students will be able to

9. Work and Potential Energy A) Overview B) Box Sliding Down a
9. Work and Potential Energy A) Overview B) Box Sliding Down a

7 Forms of Energy
7 Forms of Energy

speed
speed

... a) car suddenly stops and you strain against the seat belt b) when riding a horse, the horse suddenly stops and you fly over its head c) the magician pulls the tablecloth out from under a table full of dishes d) the difficulty of pushing a dead car f) car turns left and you appear to slide to the ri ...
Chapter11
Chapter11

... d) moment of inertia e) rotational kinetic energy ...
Chapter 07: Kinetic Energy and Work
Chapter 07: Kinetic Energy and Work

BT109 General Chemistry
BT109 General Chemistry

... Learning check • Suppose you are on an airplane travelling at constant velocity with a speed of 500 miles per hour (roughly 200 m/s) • If you throw a ball straight up, does it return to you? ...
Physics
Physics

... First Law: Object remains at rest or uniform rotation as long as no net torque (net) acts on it a. measured as the moment of inertia, I = mr2 b.  corrects for mass distribution ( = 1 for a hoop) Second Law: Fr = ma (acceleration at the rim) ...
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Work and Energy MC

Newton`s Laws - Rutgers Physics
Newton`s Laws - Rutgers Physics

... According to Newton's Second Law, the net force on a mass must change if its acceleration changes in either magnitude or direction. No net force means the body moves at constant velocity (which need not be zero). In this lab you will record the force on a body connected by a string over a pulley to ...
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Mechanics

... Generalized Velocity  Velocity is considered independent of position.  Differentials dqm do not depend on qm ...
Gravity and Gravitational Potential Energy
Gravity and Gravitational Potential Energy

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Inquiry 14.1

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Ch 13.4 - PPT - Conservation of Energy

... The Law of Conservation of Energy, continued • Energy does not appear or disappear. – Whenever the total energy in a system increases, it must be due to energy that enters the system from an external source. • Thermodynamics describes energy conservation. – For any system, the net change in energy e ...
ENERGY and WORK - Rutgers Physics
ENERGY and WORK - Rutgers Physics

... The point where the potential energy is zero can be arbitrarily chosen (since only changes in potential energy can be measured). It is conventional to make the lowest point in height the zero. Conservation of energy states that: KEi + PEi + Wnc = KEf + PEf , ...
CHAPTER XI
CHAPTER XI

... - the path of the motion can be quite different when viewed in different reference systems - inertial systems  special reference systems (systems where Newton's first law is valid) - laws of motion are the same in any two reference systems ...
Work and Energy
Work and Energy

...  The work-kinetic energy theorem allows us to think of kinetic energy as the work that an object can do while the object changes speed or as the amount of energy stored in the motion of an object.  Example: swinging the hammer in the “ringthe-bell” game has kinetic energy and can therefore do work ...
Impulse and Momentum Review
Impulse and Momentum Review

... objects, Newton’s second law says that you have to apply an unbalanced force. This implies that if there are no unbalanced forces acting on a system, the total momentum of the system must remain constant. This is another way of stating Newton’s first law, the law of inertia, discussed in chapter 4. ...
* Work (W) done by a constant force F exerted on an object through
* Work (W) done by a constant force F exerted on an object through

Example Using Conservation of Energy
Example Using Conservation of Energy

... Any instant when you can determine the energy of the object. For skier: Kinetic Energy at top Final Time Any later instant when you can determine the energy of the object. For skier: Kinetic Energy at bottom For those choices there is an in between time Time interval between Initial Time and Final T ...
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Relativistic mechanics

In physics, relativistic mechanics refers to mechanics compatible with special relativity (SR) and general relativity (GR). It provides a non-quantum mechanical description of a system of particles, or of a fluid, in cases where the velocities of moving objects are comparable to the speed of light c. As a result, classical mechanics is extended correctly to particles traveling at high velocities and energies, and provides a consistent inclusion of electromagnetism with the mechanics of particles. This was not possible in Galilean relativity, where it would be permitted for particles and light to travel at any speed, including faster than light. The foundations of relativistic mechanics are the postulates of special relativity and general relativity. The unification of SR with quantum mechanics is relativistic quantum mechanics, while attempts for that of GR is quantum gravity, an unsolved problem in physics.As with classical mechanics, the subject can be divided into ""kinematics""; the description of motion by specifying positions, velocities and accelerations, and ""dynamics""; a full description by considering energies, momenta, and angular momenta and their conservation laws, and forces acting on particles or exerted by particles. There is however a subtlety; what appears to be ""moving"" and what is ""at rest""—which is termed by ""statics"" in classical mechanics—depends on the relative motion of observers who measure in frames of reference.Although some definitions and concepts from classical mechanics do carry over to SR, such as force as the time derivative of momentum (Newton's second law), the work done by a particle as the line integral of force exerted on the particle along a path, and power as the time derivative of work done, there are a number of significant modifications to the remaining definitions and formulae. SR states that motion is relative and the laws of physics are the same for all experimenters irrespective of their inertial reference frames. In addition to modifying notions of space and time, SR forces one to reconsider the concepts of mass, momentum, and energy all of which are important constructs in Newtonian mechanics. SR shows that these concepts are all different aspects of the same physical quantity in much the same way that it shows space and time to be interrelated. Consequently, another modification is the concept of the center of mass of a system, which is straightforward to define in classical mechanics but much less obvious in relativity - see relativistic center of mass for details.The equations become more complicated in the more familiar three-dimensional vector calculus formalism, due to the nonlinearity in the Lorentz factor, which accurately accounts for relativistic velocity dependence and the speed limit of all particles and fields. However, they have a simpler and elegant form in four-dimensional spacetime, which includes flat Minkowski space (SR) and curved spacetime (GR), because three-dimensional vectors derived from space and scalars derived from time can be collected into four vectors, or four-dimensional tensors. However, the six component angular momentum tensor is sometimes called a bivector because in the 3D viewpoint it is two vectors (one of these, the conventional angular momentum, being an axial vector).
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